Abstract

We derive a set of light-cone sum rules relating the hadronic form factors relevant for B → Kπℓ+ℓ− decays to the B-meson light-cone distribution amplitudes (LCDAs). We obtain the sum rule relations for all B → K π form factors of (axial)vector and (pseudo)tensor b → s currents with a P -wave K π system. Our results reduce to the known light-cone sum rules for B → K∗ form factors in the limit of a single narrow-width resonance. We update the operator-product expansion for the underlying correlation function by including a more complete set of B-meson LCDAs with higher twists, and produce numerical results for all B → K∗ form factors in the narrow-width limit. We then use the new sum rules to estimate the effect of a non-vanishing K∗ width in B → K∗ transitions, and find that this effect is universal and increases the factorizable part of the rate of B → K∗X decays by a factor of 20%. This effect, by itself, goes in the direction of increasing the current tension in the differential B → K∗μμ branching fractions. We also discuss B → K π transitions outside the K∗ window, and explain how measurements of B → K πℓℓ observables above the K∗ region can be used to further constrain the B → K∗ form factors.

Highlights

  • Exclusive b → s decay modes have been under intense experimental and theoretical scrutiny since the era of the B-factories and the Tevatron, and have had a recent revival with the new data from the LHC

  • We find that the threshold parameter is lower than the one used in the literature for B → K ∗ form factors in the narrow-width limit

  • We construct a phenomenological model for the B → Kπ form factors and rewrite the Light-Cone Sum Rules (LCSRs) in the context of this model. Using this model we demonstrate that the narrowwidth limit leads to the well-known LCSRs for B → K ∗ form factors

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Summary

Introduction

Exclusive b → s decay modes have been under intense experimental and theoretical scrutiny since the era of the B-factories and the Tevatron, and have had a recent revival with the new data from the LHC. The various appendices include further material that complements the main part of the article: appendix A contains a collection of the LCSRs with B-meson LCDAs for the B → V form factors in the narrow-width limit. The set of sum rules given by eq (3.18) together with the OPE functions collected in appendix D are the main results of this article.

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